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NSR database version of April 11, 2024.

Search: Author = N.E.Sanderson

Found 20 matches.

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1985WO01      Phys.Lett. 150B, 79 (1985)

P.J.Woods, R.Chapman, J.L.Durell, J.N.Mo, N.E.Sanderson, R.A.Cunningham, B.R.Fulton

The Mass of 21O from the Reactions 61, 64Ni(18O, 21O)58, 61Ni

NUCLEAR REACTIONS 61,64Ni(18O, 21O), E=150 MeV; measured σ(E(21O)). 21O deduced mass excess, levels.

doi: 10.1016/0370-2693(85)90142-X
Citations: PlumX Metrics


1985WO07      Z.Phys. A321, 119 (1985)

P.J.Woods, R.Chapman, J.L.Durell, J.N.Mo, R.J.Smith, N.E.Sanderson, B.R.Fulton, R.A.Cunningham

Use of the 64Ni(36S, 34Si)66Zn Reaction to Measure the Mass of 34Si

NUCLEAR REACTIONS 64Ni(36S, 34Si), E=198 MeV; measured 34Si ion momentum spectra. 34Si deduced mass. Mass, shell models comparison.

doi: 10.1007/BF01411955
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1984DA07      Phys.Lett. 139B, 150 (1984)

T.Davinson, V.Rapp, A.C.Shotter, D.Branford, M.A.Nagarajan, I.J.Thompson, N.E.Sanderson

Coulomb and Nuclear Contribution to the Excitation of 7Li Incident on Heavy Nuclei

NUCLEAR REACTIONS 208Pb(7Li, 7Li), (7Li, 7Li'), E=68 MeV; measured σ(θ); deduced Coulomb, nuclear contribution relative importance. Coupled-channels, adiabatic model calculations.

doi: 10.1016/0370-2693(84)91233-4
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1984SH17      Phys.Rev.Lett. 53, 1539 (1984)

A.C.Shotter, V.Rapp, T.Davinson, D.Branford, N.E.Sanderson, M.A.Nagarajan

Direct Coulomb Breakup of 7Li

NUCLEAR REACTIONS 120Sn(7Li, tα), E=70 MeV; measured σ(Eα); deduced projectile breakup mechanism.

doi: 10.1103/PhysRevLett.53.1539
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1983DR06      Phys.Lett. 126B, 155 (1983)

P.V.Drumm, J.B.A.England, O.Karban, J.M.Nelson, J.M.Barnwell, N.E.Sanderson

Break-Up of Polarized 3He at 33 MeV

NUCLEAR REACTIONS 12C, 27Al, 58Ni(polarized 3He, pd), E=33 MeV; measured σ(θd, θp, Ed), analyzing power vs θd, σ(θd, θp); deduced breakup yield on 3He spin orientation. Kinematically complete experiment.

doi: 10.1016/0370-2693(83)90581-6
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1981BH02      Nucl.Phys. A363, 516 (1981)

R.K.Bhowmik, E.C.Pollacco, J.B.A.England, G.C.Morrison, N.E.Sanderson

Emission of α-Particles in Deep Inelastic Reactions Induced by 148 MeV 14N

NUCLEAR REACTIONS 12C, 27Al, 58Ni(14N, X), E=148 MeV; measured σ(fragment E, θ), fragment mass = 2-8; 12C, 27Al, 58Ni(14N, αX), E=148 MeV; measured absolute σ(E(X), θ(X), Eα, θα), αX-coin; deduced reaction mechanisms. Enriched 58Ni target.

doi: 10.1016/0375-9474(81)90271-2
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1980DU10      Phys.Lett. B94, 335 (1980)

J.L.Durell, W.R.Phillips, B.R.Fulton, J.S.Lilley, N.E.Sanderson

Comparison of Heavy Ion Transfer and Electron Scattering Measurements of the 1g9/2 Neutron Distribution in 87Sr

NUCLEAR REACTIONS 86Sr(18O, 17O), E=45, 46 MeV; measured σ(E(17O), θ). 87Sr level deduced 1g9/2 neutron rms radius.

doi: 10.1016/0370-2693(80)90891-6
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1980MO28      J.Phys.(Paris), Colloq.C-10, 243 (1980)

G.C.Morrison, R.K.Bhowmik, E.C.Pollacco, J.B.A.England, N.E.Sanderson

Alpha Emission with 10 MeV/A 14N Projectiles

NUCLEAR REACTIONS 58Ni, 27Al, 12C(14N, αX), E=148 MeV; measured σ(fragment E, θ), σ(θα, Eα), σ(Eα, θα, fragment E, θ), αX-coin, αX(θ); deduced direct mechanism for α-decay followed by deep inelastic collision.


1979BH06      Phys.Rev.Lett. 43, 619 (1979)

R.K.Bhowmik, E.C.Pollacco, N.E.Sanderson, J.B.A.England, G.C.Morrison

Pre-Emission of α Particles in Deep-Inelastic Reactions

NUCLEAR REACTIONS 58Ni(14N, 2α), (14N, αX), E=148 MeV; measured σ(Eα, E(HI), θ) for X=Li, Be, B, C, N; deduced reaction mechanism. Thick target.

doi: 10.1103/PhysRevLett.43.619
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1979FU01      Nucl.Phys. A315, 477 (1979)

B.R.Fulton, N.E.Sanderson, R.Ost, B.A.England, G.C.Morrison

Transfer Reactions and Scattering Induced by 13C on 52Cr

NUCLEAR REACTIONS 52Cr(13C, 13C'), (13C, 12B), (13C, 14C), (13C, 14N), E=105 MeV; measured σ(θ). 51V, 51Cr, 53Mn levels deduced S. Optical model, DWBA analyses. Enriched target.

doi: 10.1016/0375-9474(79)90624-9
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1978BH03      Phys.Lett. 80B, 41 (1978)

R.K.Bhowmik, E.C.Pollacco, N.E.Sanderson, J.B.A.England, G.C.Morrison

A Study of Heavy-Ion-Alpha Correlations with 11B Projectiles

NUCLEAR REACTIONS 12C(11B, αX), 58Ni(11B, αX), E=116 MeV; measured X-α(θ), differential α-multiplicities.

doi: 10.1016/0370-2693(78)90301-5
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1977RO17      Nucl.Phys. A289, 269 (1977)

S.Roman, A.K.Basak, J.B.A.England, J.M.Nelson, N.E.Sanderson, F.D.Santos, A.M.Eiro

3He D-State Effects in (d, 3He) Reactions

NUCLEAR REACTIONS 27Al(polarized d, 3He), E=12.4 MeV; measured iT11, T20, T22(θ); deduced 3He d-state contribution. Natural target.

doi: 10.1016/0375-9474(77)90032-X
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1976OS04      Nucl.Phys. A265, 142 (1976)

R.Ost, N.E.Sanderson, S.Mordechai, J.B.A.England, B.R.Fulton, J.M.Nelson, G.C.Morrison

Do Many-Particle Reactions Contribute to 'Deep-Inelastic' Peaks (Question)

NUCLEAR REACTIONS 60Ni(13C, X), E=105 MeV; measured σ(E(Z), θ), Z=3-8. 58,64Ni(13C, X), E=105 MeV; measured σ(E(Z), θ), Z=3-8, light particle coin for Li, B, Be, α, p; deduced reaction mechanism. Enriched targets.

doi: 10.1016/0375-9474(76)90120-2
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1976SA07      Nucl.Phys. A261, 93 (1976)

N.E.Sanderson, R.G.Summers-Gill

Spectroscopy of 75Se Studied with the 72Ge(α, nγ) Reaction

NUCLEAR REACTIONS 72Ge(α, nγ), E=8.1, 10.0, 13.0 MeV; measured σ(Eγ, θ), γγ-coin. 75Se deduced levels, J, π. Enriched target.

doi: 10.1016/0375-9474(76)90043-9
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1976SA14      Nucl.Phys. A266, 215 (1976)

N.E.Sanderson, M.Ivanovich

Evidence for Inelastic Processes in the 24Mg(13C, 12C)25Mg Reaction at E(lab) = 30 MeV

NUCLEAR REACTIONS 24Mg(13C, 13C), (13C, 12C), E=30 MeV; measured σ(θ). 25Mg levels deduced S. DWBA analysis. Enriched targets.

doi: 10.1016/0375-9474(76)90291-8
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1976SA26      Phys.Rev.Lett. 37, 1672 (1976)

N.E.Sanderson, A.K.Basak, J.B.A.England, J.M.Nelson, S.Roman

Investigation of d5/2-d3/2 Admixing in the Pickup Strength to the First Excited States of 22Ne and 26Mg

NUCLEAR REACTIONS 23Na, 27Al(polarized d, 3He), E=12.4 MeV; measured vector analyzing power iT11; deduced admixing in pickup strength to levels in 22Ne, 26Mg.

doi: 10.1103/PhysRevLett.37.1672
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1974HU03      Nucl.Phys. A219, 407 (1974)

S.G.Hussein, N.E.Sanderson, R.G.Summers-Gill

Low-Lying Levels of 140Pr

NUCLEAR REACTIONS 141Pr(d, t), E=16 MeV; measured σ(Et, θ). 140Ce(p, nγ), E=4.78 MeV; measured σ(Eγ, θ). 140Pr deduced levels, L(n), J, π, spectroscopic strengths. Natural, enriched targets.

doi: 10.1016/0375-9474(74)90075-X
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1974SA32      J.Phys.(London) A7, 1156 (1974)

N.E.Sanderson, J.C.Lisle, J.C.Willmott

The Level Structure of 78Kr

RADIOACTIVITY 78Rb; measured Eγ, Iγ, γγ-coin, γ(t), γγ(θ). 78Kr deduced levels, J, π, T1/2.

NUCLEAR REACTIONS 68Zn(12C, 2nγ), E=32-48 MeV; measured σ(E, Eγ, θ). 64Ni(16O, 2nγ), E=42 MeV; measured γγ-coin. 78Kr deduced levels, J, π.

doi: 10.1088/0305-4470/7/10/008
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1973SA39      Nucl.Phys. A216, 173 (1973)

N.E.Sanderson

The 76Se(d, t) Reaction and a Coriolis Coupling Theory of Anomalous States in 1g9/2 Nuclei

NUCLEAR REACTIONS 76Se(d, t), E=18, 19 MeV; measured σ(Et, θ). 75Se deduced levels, J, π, L, S. Enriched target.

doi: 10.1016/0375-9474(73)90526-5
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1971MU14      Nucl.Phys. A171, 435 (1971)

G.Murray, N.E.Sanderson, J.C.Willmott

Low-Lying Positive-Parity States in 71Ge

RADIOACTIVITY 71mGe, 71As[from 70Ge(d, p), 70Ge(d, n)]; measured T1/2, Eγ, Iγ, γγ-coin; deduced log ft. 71Ge deduced levels, J, π. Enriched target, Ge(Li) detector.

doi: 10.1016/0375-9474(71)90033-9
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